FENET Noordwijk Oct2003 MPA Steelant

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    Division of Propulsion and Aerothermodynamics

    E S T E C

    CFD Analysis of Rocket Engine

    Combustion Chambers

    J. Steelant

    TOS-MPA

    ESA - ESTEC

    Acknowledgement: R. Schmehl

    Noordwijk

    The Netherlands

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    Multi-Physics in Rocket EnginesJ. Steelant

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    Division of Propulsion and Aerothermodynamics

    E S T E C

    Aestus (Ariane 5)

    Avum (Vega)

    Oxidizer dome

    Fuel feed line

    Cooling channels

    Combustion chamber

    Injectors

    Application: Start-Up of Upper Stage Engines

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    Division of Propulsion and Aerothermodynamics

    E S T E C

    Multi-physical phenomena during start-up of LRE

    1. Priming of feed lines and domes during start-up:

    a. Waterhammer: pressure and expansion waves

    b. Phase change i.c.w. cavitation

    c. Absorption/desorption of pressurant (Helium)

    2. Injection of liquid fuel and oxidizer into the combustion chamber:

    a. Atomization evolution in near vacuum conditions

    b. Vaporization modes in near vacuum conditionsc. Droplet wall impact and break-up processes

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    Multi-Physics in Rocket EnginesJ. Steelant

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    Division of Propulsion and Aerothermodynamics

    E S T E C

    Study: priming effects

    in vacuum

    1. Waterhammer with phase change

    2. Unsteady injection process

    3. Checking coupling with CC-

    instabilities modes

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    Division of Propulsion and Aerothermodynamics

    E S T E C

    CFD-Analysis (1/3)1. Geometrical aspects

    - axisymmetric fuel dome with annular injector slits

    - spatial : 20K nodes; temporal: 1 sec

    P9D1

    P_cent

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    Division of Propulsion and Aerothermodynamics

    E S T E C

    CFD-Analysis (2/3)2. Numerical aspects

    - Spatial: 3rd order Smart-scheme

    - Time: backward Euler (1st order)

    - Solver: Pressure-Correction method

    3. Physical modelling:

    - Transient laminar and isothermal Navier-Stokes equations

    - Vapor transport equations:

    MMH vaporization/condensation & presence of

    non-condensable gas.

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    Division of Propulsion and Aerothermodynamics

    E S T E C

    CFD-Analysis (3/3)Vapor transport equation: f = vapour mass fraction

    expressions for Re and Rcderived from Rayleigh-Plessetequation with:

    where Ce, Cs = phase change rate coefficients

    = surface tension

    psat = saturation pressure

    Vch = characteristic velocity

    feRRffu

    t

    f+=+

    )()(

    r

    )1(3

    2f

    ppVCR

    l

    satlv

    chee

    =

    f

    ppVCR

    l

    sat

    lvch

    cc

    =

    3

    2

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    Division of Propulsion and Aerothermodynamics

    E S T E C

    Evolution of void fraction

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    Division of Propulsion and Aerothermodynamics

    E S T E C

    Spectral analysis: CFD result for 50mg N2/kg MMH

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    Division of Propulsion and Aerothermodynamics

    E S T E C

    Study: injection processes in near vacuum

    1. Thermodynamic behaviour of a liquid jet into near vacuum

    2. Atomization behaviour of a liquid jet in near vacuum

    3. Transport and deformation of atomized jets (spray)

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    Division of Propulsion and Aerothermodynamics

    E S T E C

    Thermodynamic behaviour in near vacuum: flashing

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    Division of Propulsion and Aerothermodynamics

    E S T E C

    Flash vaporization model

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    Division of Propulsion and Aerothermodynamics

    E S T E C

    Flash vaporization in near vacuum

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    Division of Propulsion and Aerothermodynamics

    E S T E C

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    Division of Propulsion and Aerothermodynamics

    E S T E C

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    Division of Propulsion and Aerothermodynamics

    E S T E C

    Transport and deformation of atomized jets

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    Division of Propulsion and Aerothermodynamics

    E S T E C

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    Division of Propulsion and Aerothermodynamics

    E S T E C

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    Division of Propulsion and Aerothermodynamics

    E S T E C

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    Division of Propulsion and Aerothermodynamics

    E S T E C

    Wall impact, deposition and rebounce

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    Division of Propulsion and Aerothermodynamics

    E S T E C

    Wall deposition rate

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    Division of Propulsion and Aerothermodynamics

    E S T E C

    Conclusion

    1. Multiphysical processes in LRE

    a. Phase change icw waterhammer, cavitation, absorption,during priming

    b. Processes during injection Flashing atomization & vaporization

    Primary and secondary break-up of jets

    Wall deposition/interaction of droplets

    2. Modelling and numerical simulation allows qualitative and/orquantitative analysis of processes difficult to analyseexperimentally